We first examine the momentum density, with the results on the triangular lattice in Fig. REF . Both spin-species have momentum density close to unity beneath their respective Fermi momenta and close to zero above. A breached superfluid [1]}, [2]}, [3]} would have the majority species exhibit depletion at the minority species Fermi momentum and a system crossing the Chandrasekhar-Clogston limit [4]}, [5]} would have finite momentum density of the minority species at the majority species Fermi momentum, so it is clear that the system has not relaxed into either of those possible states. Knowing this, we can now move on to study the emergence of superconductivity by examining the condensate fraction.
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